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Composite Gel Polymer Electrolyte for Improved Cyclability in Li-Oxygen Batteries Amir Chamaani, Meer Safa, Neha Chawla, and Bilal El-Zahab ACS Appl. Mater. Interfaces, Just Accepted Manuscript • DOI: 10.1021/acsami.7b08448 • Publication Date (Web): 06 Sep 2017 Downloaded from http://pubs.acs.org on September 7, 2017
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Composite Gel Polymer Electrolyte for Improved Cyclability in Li-Oxygen Batteries Amir Chamaani, Meer Safa, Neha Chawla, and Bilal El-Zahab* Department of Mechanical and Materials Engineering, Florida International University, Miami, FL, 33174, USA *
Corresponding author.
Corresponding author. Tel.: +1-305-348-3558; Fax: +1-305-348-1932. E-mail address:
[email protected] (B. El-Zahab).
Keywords: Li-O2
battery,
Electrolyte
stability,
Composite
gel
polymer
electrolyte,
electrolyte
decomposition, electrochemical impedance spectroscopy, lithium transference number, glass microfillers.
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Abstract: Gel polymer electrolytes (GPE) and composite GPE (cGPE) using one-dimensional microfillers have been developed for their use in lithium-oxygen batteries. Using glass microfillers, tetragylme solvent, UV curable polymer, and lithium salt at various concentrations, the preparation of cGPE yielded free-standing films. These cGPE, with 1% by weight of microfillers, demonstrated increased ionic conductivity and lithium transference number over GPE at various concentrations of lithium salt. Improvements as high as 50% and 28% in lithium transference number were observed for 0.1 and 1.0 mol·kg-1 salt concentrations, respectively. Lithium-oxygen batteries containing cGPE similarly showed superior charge/discharge cycling for 500 mAh.g-1 cycle capacity with as high as 86% and 400% increase in cycles for cGPE with 1.0 and 0.1 mol·kg-1 over GPE. Results using electrochemical impedance spectroscopy, Raman spectroscopy, and scanning electron microscopy revealed that the source of the improvement was the reduction of the rate of lithium carbonates formation on the surface of the cathode. This reduction in formation rate afforded by cGPE-containing batteries was possible due to the reduction of the rate of electrolyte decomposition. The increase in solvated to paired Li+ ratio at the cathode, afforded by increased lithium transference number, helped reduce the probability of superoxide radicals reacting with the tetraglyme solvent. This stabilization during cycling helped prolong the cycling life of the batteries.
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Introduction The transition from fossil fuels to renewable resources has created more demand for energy storage devices. Lithium-ion (Li-ion) batteries have been widely used during the last two decades to fulfill this need, especially in electronics and transportation applications. Although many studies reported Li-ion batteries operating near their theoretical capacities, they remain insufficient for emerging applications such as electric vehicles1. Therefore, an increasing amount of research has been devoted to developing new chemistries beyond Li-ion batteries. Li-O2 batteries have attracted much attention due to their high theoretical energy densities approaching that of gasoline2. Li-O2 batteries typically consist of a lithium metal anode, porous air cathode covered by carbonaceous materials, and a Li+ ion conducting electrolyte. In a discharge process, Li2O2 is deposited on the surface of the cathode via an oxygen reduction reaction (ORR) and removed from the surface of the cathode via an oxygen evolution reaction (OER) during the charge process2. Li-O2 batteries, however, are still in their infancy and several fundamental challenges remain to be addressed before their commercialization3. Advanced chemical and electrochemical techniques have revealed that, to some degree, all components of LiO2 battery undergo undesirable chemical/electrochemical changes during repeated discharge/charge cycling, contributing to the reduced cyclability4–6. For example, the carbon cathodes can react with Li+ and oxygen during OER7, and the oxygen crossover from the air cathode can corrode the lithium anode8. Protecting the lithium metal anode9,10 and replacing the carbonaceous cathode materials11 have been some of the suggested solutions to improve the Li-O2 battery performance. However, according to recent reports, the electrolyte remains as the leading cause for rapid capacity fading and poor
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cyclability in Li-O2 batteries12–14. Commonly carbonate-based solvents used in Li-ion batteries have been shown to be unstable during the ORR process15. Consequently, etherbased electrolytes have been suggested for Li-O2 battery applications16,17. Nonetheless, the stability of ether-based electrolytes remains a concern and recent studies reported on the reactivity between superoxide radical species formed during charge/discharge with the ether-based solvents18–20. The hydrogen abstraction from methylene groups in ether-based solvents by superoxide radical species and subsequent reactions can cause solvent decomposition and the formation of lithium carbonates. The progressive formation of these insulating decomposition products on the surface of the cathode yields high cell polarization, thus causing poor cyclability7,14,18. Functionalized ether-based solvents (e.g. 2,3-dimethyl-2,3-dimethoxybutane
(DMDMB)
and
tri(ethylene
glycol)-substituted
trimethylsilane (1NM3)) have been proposed to eliminate the possibility of methylene hydrogen abstraction14,21. Increasing the concentration of lithium salt in electrolytes was also shown to improve the performance of Li-O2 batteries22–24. The appropriate Li+ solvation with solvent molecules may increase the favorable accessibility of superoxides to Li+ by increasing the salt concentration, which in turn mitigates the electrolyte decomposition22–24. Gel polymer electrolytes (GPE) consisting of liquid electrolyte and polymer has been successfully used in lithium-ion batteries due to their high ionic conductivity and mechanical stability25–27. Recently, GPE with different electrolytes and polymers have also been developed for Li-O2 battery applications28–32. It has been reported that GPE improve the performance of Li-O2 batteries by reducing the electrolyte evaporation, and preventing the lithium corrosion caused by oxygen crossover from air cathode30,32,33.
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Inorganic filler materials have been widely incorporated into electrolytes and were shown to yield an increase in ionic conductivity and Li+ transference number34–36. Croce et. al37 showed that the Lewis acid groups on the surface of ceramic fillers in composite polymer electrolytes strongly adsorb the anions of the lithium salt and enhance its salt dissociation. Bhattacharyya and Maier38 also observed the same anion adsorption behavior of ceramic fillers in non-aqueous liquid electrolytes. Incorporation of various ceramic fillers in different electrolytes have also been explored for Li-O2 battery applications32,39–44. It has been shown that the inorganic fillers can improve the performance of Li-O2 batteries by stabilizing the interfacial resistance and preventing lithium anode corrosion. In this study, we investigate the incorporation of one-dimensional glass microfillers into glymebased GPEs on reducing the formation of parasitic electrolyte decomposition byproducts in LiO2 batteries. Charge/discharge cycling, EIS, SEM, and Raman spectroscopy have been used to assess the performance improvement of composite gel electrolyte (cGPE) containing batteries.
Materials and Method Materials Ethoxylated trimethylolpropane triacrylate (ETPTA, Mw=428), 2-hydroxy-2-methyl-1phenyl-1-propanon (HMPP, Photo-initiator), lithium bis(trifluoromethane) sulfonamide (LiTFSI), tetraethylene glycol dimethyl ether (TEGDME), N-Methylpyrrolidine (NMP), Polyvinylidene fluoride (PVDF), multiwalled carbon nanotubes (CNTs) and Whatman glass microfiber filters (Binder free, Grade GF/B) were purchased from Sigma-Aldrich. A carbon cloth gas diffusion layer (CCGDL) was obtained from FuelCell Earth. Celgard 2400 polypropylene separator was also obtained from Celgard.
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Gel polymer and Composite Gel Polymer Electrolyte Preparation TEGDME solvent was dried over 4Å molecular sieve in Ar-filled glovebox. Liquid electrolyte solutions were prepared by dissolving different concentrations of LiTFSI salt (0.1, 1.0 and 3.0 mol·kg-1) in TEGDME. The GPE and cGPE with nonporous glass microfibers were prepared following the procedure detailed in our previous work44. Briefly, GPE were prepared by mixing of ETPTA monomer into liquid electrolytes (0.1, 1, and 3 mol·kg-1) solution (80:20 wt.% of ETPTA/liquid electrolyte with 1:99 by weight HMPP: ETPTA monomer content as a curing agent). The cGPE preparation followed the same procedure with the addition of 1 wt.% of glass microfibers. The mixture solutions were cast on glass slides inside Ar-filled glovebox and were irradiated (365 nm) for 10 minutes which formed free-standing and flexible films of 150-200 µm in thickness. Figure S1 shows photographs of GPE and cGPE with 1mol·kg-1 LiTFSI salt. Cathode Preparation and Cell Assembly Cathodes were prepared by coating CNTs/PVDF (90:10 wt.% in NMP) slurry on the carbon cloth gas diffusion layer (CCGDL) and dried at 120°C overnight. The loading of CNTs was 0.5 ± 0.03 mg·cm-2. As-prepared GPE and cGPE were placed between a lithium anode and presoaked cathode with liquid electrolytes. For a comparative experiment, the Li-O2 cells with liquid electrolytes were also assembled using presoaked separators with liquid electrolytes. All electrolyte preparations and cell assembly were performed inside an Ar-filled glove box ( 99.994%) via gas manifolds containing humidity-resistant tubing and rested under oxygen for 5 hours before testing. Characterization The ionic conductivity (σ) of GPE and cGPE was calculated following the equation σ=L/A·R, where L is the thickness, A is the area, and R is the bulk resistance of the electrolytes obtained using electrochemical impedance spectroscopy (EIS). Li+ transference number (tLi+) was determined using the Bruce-Vincent method by applying a 10 mV DC polarization signal to determine the initial and steady-state currents combined with the impedance determination of the cell before and after polarization45. Figure S2 (supporting information) shows typical chronoamperometric curves of Li/GPE or cGPE /Li along with the EIS spectra collected before and after DC polarization for the salt concentration of 0.1 mol·kg-1. Galvanostatic charge/discharge tests were performed using MTI battery tester at the constant current density of 250 mA·g-1 within the voltage range of 2.0–4.5 V. In-situ EIS measurements were also conducted using a Gamry Reference 600 in the frequency range of 100 kHz to 10 mHz using 10% of DC discharge current during cycling test. All charge/discharge and EIS studies were carried out at 25oC. After cycling, the oxygen cathodes were recovered from the cells under Ar and were further characterized using Raman spectroscopy (BaySpec’s Nomadic™, 532 nm), X-ray diffraction (XRD, Bruker GADDS/D8 with MacSci rotating Molybdenum anode (λ= 0.71073 Å)) and scanning electron microscopy (SEM, JEOL 6330F). Raman spectroscopy was also performed on the liquid electrolytes, GPEs and cGPEs with different Li salt concentrations. All electrolyte samples were placed in airtight rectangular quartz cuvettes under argon then examined by Raman spectrometer (BaySpec’s Nomadic™, 532 nm).
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Each spectrum was recorded with the exposure time of 20 s using 10x objective lens at 25°C.
Results and Discussion The ion transport properties of the GPE and cGPE prepared using various concentrations of lithium salt were evaluated using their corresponding methods described in the Materials and Methods. Table 1 summarizes the ionic conductivity (σ) and lithium transference number at room temperature (25°C). Table.1. Summary of ionic conductivity and Li+ transference number of GPE and cGPE at different salt concentrations. Electrolyte films
Transference Number tLi+
Ionic Conductivity σ (mS·cm-1)
GPE-0.1 mol·kg-1 GPE-1.0 mol·kg-1 GPE-3.0 mol·kg-1 cGPE-0.1 mol·kg-1 cGPE-1.0 mol·kg-1
0.40±0.02 0.50±0.03 0.54±0.02 0.60±0.02 0.64±0.02
0.13±0.02 1.02±0.05 0.68±0.02 0.35±0.05 1.40±0.02
cGPE-3.0 mol·kg-1
0.55±0.03
0.70±0.02
The ionic conductivity of GPE was shown to increase with increasing salt concentration from 0.1 mol·kg-1 to 1.0 mol·kg-1 due to the increase in the number of free ions. However, as the salt concentration increases to 3.0 mol·kg-1, the ionic conductivity decreases as previously reported46. This decrease is mostly due to a drop in ion mobility caused by higher viscosity of the liquid electrolyte soaking the polymer matrix47,48. The lithium transference number for GPE showed an increasing pattern with increasing salt concentration and followed similar behavior of glyme-based liquid electrolytes and
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polyacrylate based GPE47,48. In Glyme-based electrolytes containing LiTFSI salt, the increase in the salt concentration was shown to decrease the ionic association49, and in turn, increases the Li+ transference number. The effect of the glass microfillers was demonstrated in increases in both σ and tLi+ for the cGPE. This increase was owed to the immobilization of the TFSI-, likely through interactions between Lewis acid groups on filler’s surface and TFSI- anions36,50,51. This ion-ceramic interaction yields an improvement in the ion pair dissociation and increases Li+ dissociation50. At an optimized filler’s content of 1 wt.%44, a percolating network of glass microfibers is formed providing Li+ transportation pathways. This increase was not apparent for the 3.0 mol·kg-1 cGPE, indicating insufficient surface groups for the immobilization of TFSI-. This indicates that the effect of surface ion adsorption is reduced in environments with abundance of free ions52. Therefore, with a fixed filler’s loading, the effect of fillers was only apparent in cGPE with salt concentrations below a certain threshold, that once exceeded, the effect of fillers at that loading is reduced due to excessive amounts of ions in the solution. Raman spectroscopy study was performed on liquid electrolytes, GPEs, and cGPEs to further investigate the interaction of ETPTA polymer and the microfillers with LiTFSI salt. Figure S3 (supporting information) shows that a Raman spectrum of TFSI- anion which is assigned to the contraction and expansion mode of S-N coupled with CF3 bending53. This Raman spectrum also represents the Li+ and TFSI- association54. The Raman shift between 736-742 cm-1 is assigned to the unbounded TFSI- (free anion or solvent separated ion pairs (SSIPs))54,55 and Raman shift ≥ 744 cm-1 show the bounded TFSI- (contact ion pairs (CIPs) and ion aggregates)54,55. As shown in Figure S3 (supporting information), for all electrolyte samples, the addition of
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ETPTA polymer to liquid electrolytes with different salt concentrations does not change the shape of the TFSI- Raman spectrum as they all exhibit two distinct Raman shifts for unbounded and bounded TFSI- confirming that ETPTA polymer does not have any iontrapping ability26 and acts merely as an inert polymer. Furthermore, the addition of 1 wt.% glass microfillers to the GPEs at 0.1 and 1 mol·kg-1 LiTFSI shows that the dissociation level of LiTFSI increases as the Raman shift of bounded TFSI- (shoulder ≥ 744 cm-1) was significantly reduced. However, cGPE at 3 mol·kg-1 LiTFSI salt concentration indicates no significant changes in Raman shift of bounded TFSI-. These results are completely in agreement with reported transference numbers. To examine the impact of glass microfillers on the performance of Li-O2 batteries, charge/discharge cycling tests were performed at 250 mA·g-1 for a cycle capacity of 500 mAh·g-1 in a voltage window of 2.0-4.5 V. Figure 1 depicts the voltage profiles of GPEand cGPE-containing Li-O2 batteries using various salt concentrations up to the first cycle after their failure (first cycle with less than 500 mAh·g-1). Cells using GPE-0.1 mol·kg-1 ran for 12 discharge cycles compared to the GPE-1.0 mol·kg-1 and GPE-3.0 mol·kg-1 that ran for 29 and 40 cycles, respectively. This increase in cyclability with increased salt content has not been previously observed for GPE, but was previously reported for liquid electrolytes22,23. Furthermore, cells using cGPE-0.1 mol·kg-1 and cGPE-1.0 mol·kg-1 showed 49 and 54 consecutive discharge cycles, respectively compared to cGPE-3.0 mol·kg-1 with 43 discharge cycles. Using microfillers substantially improved the cyclability performance of Li-O2 battery by 400% and 86% more cycles compared to their GPE counterparts for 0.1 and 1.0 mol·kg-1, respectively. However, no significant improvement of cGPE over GPE was observed for 3.0 mol·kg-1. This observation is
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consistent with the transference number improvements due to the inclusion of microfillers, proving the importance of Li+ transport properties of electrolytes on the LiO2 battery performance44,56,57.
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Figure 1. Voltage profile of Li-O2 batteries using GPE and cGPE with different salt concentrations with a limited capacity of 500 mAh·g-1 per cycle at current density of 250 mA·g-1. (The voltage profiles of GPE and cGPE (1 mol·kg-1) were obtained from our previous work44) The Li-O2 cells using liquid electrolytes also show 10, 30 and 40 cycles of 500 mAh·g-1 charge/discharge at 250 mA·g-1 in voltage windows of 2.0-4.5 V. Similarity between the cyclability of cells using liquid electrolytes and GPEs indicates that the ETPTA does not have any significant effect on the Li-O2 battery performance. The formation of Li2O2 was confirmed by performing Raman spectroscopy on the surface of cathodes after one discharge cycle of 500 mAh·g-1. From Figure S4 (supporting information), all spectra show a Raman shift at ~800 cm-1 corresponding to the Li2O258. The presence of Li2O2 confirms that the discharge capacities of all Li-O2 batteries are mainly due to ORR. As previously suggested by Noked et. al59, the contribution of background discharge capacity of the CNTs-free CCGDL substrate to the total capacity of Li-O2 batteries per cycle was measured to be less than 1% (see supporting information, figure S5). EIS has been recently used in metal-O2 battery systems to conduct the in-situ determination of cell degradation mechanisms60–63. In this study, EIS was performed during cycling after discharge at OCV to evaluate the electrochemical behavior of GPE and cGPE. Figure 2a shows an example of a Nyquist plot of a Li-O2 cell under oxygen using GPE-1.0 mol·kg-1 after the discharge of the first cycle, 10th, 25th, and 29th (failure) cycles. The Nyquist plots consisted of a semicircle corresponding to the interfacial resistance (Rint) between the electrolyte (GPE or cGPE) and the electrodes, and a
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Warburg-like linear region followed by a rise, which are in agreement with other metalO2 EIS spectra at non-faradic conditions60–62. Transmission line model (TLM) has been used to determine the impedance behaviour of the porous electrodes in Li-ion and metalO2 batteries60,61,64. In TLM, it is assumed that the Warburg-like linear region corresponds to the resistance of lithium-ion migration (Rion) at the cathode60,61. Similar EIS behaviors were observed for GPE and cGPE at the other salt concentrations.
Figure 2. (a) Typical Nyquist plots of Li-O2 batteries using GPE with 1.0 mol·kg-1 salt concentration at OCV after first and failure cycle along with cycle 10th and 25th cycle (inset: shows close-up of Nyquist plots showing changes in interfacial resistances during cycling). (b) Transmission line model used to interpret the resistances of Nyquist plots.
The rise at low frequencies (less than 100 mHz) in the EIS spectra is consistent with the capacitive signal originated from the porous cathode60,61. Using TLM model, the Rion could be estimated by the projection of the Warburg-like line on the impedance abscissa
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(Rion/3)64,65 (Figure 2b). The electrolyte resistance (Rb) and interfacial resistance (Rint) were also obtained by analysing the real resistances of the semicircle of the EIS spectra at the high- and mid-frequency, respectively (Figure. 2b). As can be seen from Figure 2a, the Warburg-like line’s slope steadily declines upon cycling. Furthermore, the diameter of the semicircle (Rint) is decreased in cycles 1 to 10, and then increased in cycles 10 and higher (Figure 2a inset). Figure 3 shows the change of resistances Rion, Rb and Rint versus discharge cycle numbers. Rion was the dominant resistance in the cells which indicates that the increase in the resistance of cathode is the main cause for the failure. Shui et. al66 and Knudsen et. al61 also reported that the deactivation of the cathode was a major culprit in Li-O2 battery failure. The increase in Rion upon cycling indicates a physical pore clogging within the porous cathodes caused by irreversible charge/discharge products deposition hindering Li+ transport inside the cathode67. Tracking Rion of cells using GPE- and cGPE-containing batteries at various salt concentrations (Figure 3) shows that for 0.1 and 1.0 mol·kg-1 cGPE-containing batteries had lower Rion after the first discharge cycle and remained consistently lower than in their GPE-containing counterparts. In addition, the rate of growth of the Rion also increased at a slower rate than for GPE-containing batteries, indicating that pore-clogging depositions mainly in the cathode was less problematic in batteries containing the cGPE. However, for the GPE and cGPE with 3.0 mol·kg-1 no significant reduction in Rion growth was observed, which again suggests that the effect of the microfillers at this concentration was ineffective.
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Figure 3. The change of resistances of Li-O2 batteries using GPE and cGPE with different salt concentrations during cycling up to their failure.
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This observation is consistent with the transference number and cycling comparisons previously discussed. To investigate the composition of the pore-clogging deposits, Raman spectroscopy was performed on the surface of cycled cathodes. Figure 4 shows the Raman spectra of cathodes using the GPE and cGPE at 0.1 and 1.0 mol·kg-1 recovered from Li-O2 batteries after the 12th and the 29th discharge cycles (the failure cycles of GPE-containing batteries), respectively. Cathodes of GPE-containing batteries show pronounced Raman shifts at 1082 cm-1, which correspond to the formation of lithium carbonates58,68. Conversely, the cathodes recovered from cGPE-containing batteries cycled under the same conditions and for the same number of cycles show less pronounced Raman shifts at 1082 cm-1, indicating lesser formation of lithium carbonates. These results confirm both the location (cathode) and the nature (lithium carbonates) of the depositions leading to the pore-clogging and consequently the growth of Rion. The presence of lithium peroxides and lithium carbonates were also confirmed by XRD (Figure S6, supporting information). Lithium carbonates can be formed by decomposition of carbon cathodes and electrolytes4,18,20. However, the formation of carbonate species during cycling of Li-O2 batteries using tetragylme-based electrolyte is suspected to be dominated by electrolyte decomposition7. This suggest that the addition of glass microfibers to the GPEs at 0.1 and 1.0 mol·kg-1 reduces the electrolyte decomposition.
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Figure 4. Raman spectra of cycled cathodes after discharge using GPEs and cGPEs with 0.1 and 1 mol·kg-1 salt concentration at cycle number where the batteries using GPEs fails (cycle 12th for 0.1 mol·kg-1 and cycle 29th for 1 mol·kg-1).
The cathodes of cells after the failure discharge cycle (the failure cycles of GPEcontaining batteries) were recovered and visually inspected using SEM. In figure 5, the cathode of batteries containing cGPE-1.0 mol·kg-1 shows toroid-shaped discharge products (mostly Li2O2) covered by some fuzzy needle-like structures, previously reported as lithium carbonates69. Figure S7 also shows the toroid-shaped Li2O2 discharge products in higher magnification. In contrast, cathode of batteries using GPE-1.0 mol·kg1
are mostly covered by the fuzzy needle-like structures and almost completely burying
the toroid-shaped discharge products. This confirms the formation of the passivating
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lithium carbonates layer on the cathode. The continuous formation of these insulating lithium carbonates yielded large voltage hysteresis with increase in cycling (Figure 1).
Figure 5. SEM micrograph of cycled cathodes in Li-O2 batteries using cGPE (a) and GPE (b) with 1.0 mol·kg-1 salt concentration after the failure discharge cycle.
The impact of cycling on the interfacial resistance (Rint) in the Li-O2 batteries is shown in figure S8 (supporting information). The Rint decreases in the initial cycles before it starts to grow in later cycles until the failure cycle. A similar phenomenon was also observed in our previous study44. As previously observed, the interfacial resistance of Li-O2 batteries is initially governed by anode/electrolyte interface61,67. Hence the decrease in the Rint at initial cycles is mainly related to the dissolution of the passivation film on the anode/electrolyte films interface43. However, the increase in Rint in later cycles could be related to the accumulation of irreversible charge/discharge by-products on the anode/electrolyte70 and cathode/electrolyte interfaces67. Yi et. al40,41 also showed that the formation of lithium carbonates by-products on the cathode/electrolyte interface could
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increase the interfacial resistance in Li-O2 batteries during cycling. The addition of microfillers (especially in 0.1 and 1.0 mol·kg-1 salt concentration) maintained a lower Rint throughout the cycling, and can be credited to stabilizing the electrolyte and reducing its decomposition rate. From the results obtained using the charge/discharge cycling, EIS, and Raman spectroscopy, the improvement in Li+ transport properties, especially lithium transference number correlated strongly with the improvement in cyclability of Li-O2 batteries, mainly due to the stabilization of the electrolyte. At the cathode, the main source of instability of the electrolyte during discharge is the reaction of superoxide radicals with the glymebased solvent molecules. Thotiyl et. al confirmed the prevalence of this reaction during discharge by tracking the
13
C isotopic species in the decomposition products7. These
superoxide radicals under ideal conditions would be reacting with the Li+ to yield Li2O2. However, in electrolytes with inefficient Li+ transport properties, the ratio of solvated Li+ to loosely bound ion pairs composed of solvated Li+ and TFSI- is reduced48,49, which in turn, increases the probability of the reaction of superoxide radical with the solvent23,24 and promotes the electrolyte decomposition. Therefore, since an increase in transference properties of the electrolyte is associated with higher ratio of solvated Li+, GPE and cGPE with improved transference numbers help reduce electrolyte degradation. The degradation and eventual formation of lithium carbonates can therefore be reduced in Li-O2 batteries using higher transference number electrolytes such the cGPE presented in this work.
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Conclusion In this study, gel polymer electrolytes (GPE) and glass microfillers-containing composite GPE (cGPE) were developed for their use in Li-O2 batteries. Using various concentrations of lithium salt, it was observed that the resulting cGPE had improved lithium transport properties. Li-O2 batteries containing cGPE cycled up to 5-fold more cycles of 500 mAh·g-1 capacity per cycle compared to batteries containing GPE. This improvement was determined to be due to the reduction of the growth of ionic resistances in the cathode and its electrolyte interface. This resistance was traced back to the formation of lithium carbonates on the cathode due to the degradation of the tetraglyme-based solvent in the electrolyte. We theorize that the improved lithium transference of the cGPE increased the ratio of solvated to coupled Li+ which reduced the probability of superoxide radicals reacting with the tetraglyme-based solvent during cycling.
ASSOCIATED CONTENT Supporting Information Photographs of GPE and cGPE with 1 mol·kg-1 LiTFSI salt concentration; Chronoamperometric curves of Li/GPE and cGPE /Li cell after 10 mV of DC polarization at 25°C where the electrolyte films contain 0.1 mol·kg-1 LiTFSI salt along with electrochemical impedance spectra before and after polarization; Raman spectra of Liquid electrolytes, GPEs and cGPEs with various LiTFSI salt concentrations showing Raman shifts of bounded and unbounded TFSIanions; Raman spectra of 500 mAh·g-1 predischarged cathodes using GPE and cGPE with different salt concentration confirming the presence of Li2O2; Voltage profiles of Li-O2 batteries
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using CNTs-free CCGDL in full discharge mode and CCGDL with 0.5 mg of CNTs in 500 mAh·g-1 discharge mode at 125µA current; XRD patterns of cathodes using GPE and cGPE (1 mol·kg-1 LiTFSI salt concentration) showing the presence of lithium peroxide and lithium carbonates; SEM micrograph of toroid-shaped Li2O2 discharge products; The evolution of interfacial resistance (Rint) of cells suing GPE and cGPE with different salt concentration during cycling up to their failure cycles versus selected cycle number
AUTHOR INFORMATION Corresponding Author *
Tel.: +1-305-348-3558; Fax: +1-305-348-1932. E-mail:
[email protected] Acknowledgment The authors acknowledge Dr. Alexander Franco of the Advance Materials Research Institute (AMERI) for the assistance in electron microscopy and Prof. N. Pala’s group for their help in Raman spectroscopy measurements. The authors also thank Dr. Vadym Drozd of the Center for the Study of Matter at Extreme Conditions (CeSMEC) for his assistance in the XRD analyses. A.C. also acknowledges the financial support of FIU Dissertation Year Fellowship.
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